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Volumn 64, Issue 24, 2001, Pages

Theory of combined exciton-cyclotron resonance in a two-dimensional electron gas: The strong magnetic-field regime

Author keywords

[No Author keywords available]

Indexed keywords

ARTICLE; CYCLOTRON; DENSITY; DYNAMICS; ELECTRON; EXCITATION; GAS; MAGNETIC FIELD; PHOTON; ROTATION; THEORY;

EID: 0035894505     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.64.241101     Document Type: Article
Times cited : (14)

References (19)
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    • Proceedings International Conference on Electronic Properties of Two-Dimensional Systems (EP2DS-14, Prague, Czech Republic, 2001), Physica E (to be published)
    • Proceedings International Conference on Electronic Properties of Two-Dimensional Systems (EP2DS-14, Prague, Czech Republic, 2001), Physica E (to be published).
  • 4
    • 0001545344 scopus 로고    scopus 로고
    • references therein.
    • S. Glasberg et al., Phys. Rev. B 59, R10425 (1999), and references therein.
    • (1999) Phys. Rev. B , vol.59
    • Glasberg, S.1
  • 6
    • 85038970481 scopus 로고    scopus 로고
    • Ref. 1 (cond-mat/0106277), and references therein.
    • H. A. Nickel et al., in Ref. 1 (cond-mat/0106277), and references therein.
    • (1996) Phys. Rev. B , vol.53 , pp. 12593
    • Nickel, H.A.1
  • 13
    • 85038935195 scopus 로고    scopus 로고
    • A.B. DzyubenkoPhys. Rev. B (to be published), cond-mat/0107611.
    • Dzyubenko, A.B.1
  • 14
    • 85038947964 scopus 로고    scopus 로고
    • This is quantitatively correct at low magnetic fields, when the bound complex rotates in B as a whole
    • This is quantitatively correct at low magnetic fields, when the bound complex rotates in B as a whole.
  • 15
  • 16
    • 0000924216 scopus 로고
    • Zh. Éksp. Teor. Fiz. 78, 1167 (1980)
    • I.V. Lerner and Yu.E. Lozovik, Zh. Éksp. Teor. Fiz. 78, 1167 (1980) [Sov. Phys. JETP 51, 588 (1980)].
    • (1980) Sov. Phys. JETP , vol.51 , pp. 588
    • Lerner, I.V.1
  • 17
    • 85038887358 scopus 로고    scopus 로고
    • This conclusion is reached for a strictly-2D system in the limit of high magnetic fields. It is applicable to quasi-2D systems at finite fields—as long as no bound (Formula presented) states with (Formula presented) appear in the first electron LL
    • This conclusion is reached for a strictly-2D system in the limit of high magnetic fields. It is applicable to quasi-2D systems at finite fields—as long as no bound (Formula presented) states with (Formula presented) appear in the first electron LL.


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